Work in the real space, consistent with the specified real step coefficients. First approximate an integrable function by a finite-valued measurable function with bounded support. Truncate its domain to and its values to ; the error tends to zero by integrability. Quantize those remaining values in intervals of mesh , producing a simple function with finite-measure Borel sets and error at most on the truncated domain. Thus can be made arbitrarily small.
For each , use the allowed approximation by a finite union of intervals , choosing the symmetric-difference errors so
These unions can be written as finite disjoint bounded intervals, and changing endpoints to the required half-open convention changes only a null set. The function is therefore a step function of the specified form, and
Combining the two approximations proves the step functions are dense in . In the complex version of , the same argument applies to real and imaginary parts when complex step coefficients are allowed.

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